Qin-Song Zhou, Zi-Yue Bai, Jun-Zhang Wang, Hao Xu, Xiang Liu
{"title":"解码ρ介子态在解释e+e−→a2(1320)π数据和其他反应中的作用","authors":"Qin-Song Zhou, Zi-Yue Bai, Jun-Zhang Wang, Hao Xu, Xiang Liu","doi":"10.1103/pdfh-mk79","DOIUrl":null,"url":null,"abstract":"Recently, the BESIII Collaboration observed a ρ</a:mi></a:math>-like structure <c:math xmlns:c=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><c:mi>Y</c:mi><c:mo stretchy=\"false\">(</c:mo><c:mn>2044</c:mn><c:mo stretchy=\"false\">)</c:mo></c:math> in <g:math xmlns:g=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><g:msup><g:mi>e</g:mi><g:mo>+</g:mo></g:msup><g:msup><g:mi>e</g:mi><g:mo>−</g:mo></g:msup><g:mo stretchy=\"false\">→</g:mo><g:msub><g:mi>a</g:mi><g:mn>2</g:mn></g:msub><g:mo stretchy=\"false\">(</g:mo><g:mn>1320</g:mn><g:mo stretchy=\"false\">)</g:mo><g:mi>π</g:mi></g:math>, suggesting that <l:math xmlns:l=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><l:mi>Y</l:mi><l:mo stretchy=\"false\">(</l:mo><l:mn>2044</l:mn><l:mo stretchy=\"false\">)</l:mo></l:math> may be a candidate of vector meson <p:math xmlns:p=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><p:mi>ρ</p:mi><p:mo stretchy=\"false\">(</p:mo><p:mn>2</p:mn><p:mi>D</p:mi><p:mo stretchy=\"false\">)</p:mo></p:math> by comparing resonance parameters. However, the theoretical prediction for the combined branching ratio <t:math xmlns:t=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><t:msub><t:mi mathvariant=\"normal\">Γ</t:mi><t:mrow><t:msup><t:mi>e</t:mi><t:mo>+</t:mo></t:msup><t:msup><t:mi>e</t:mi><t:mo>−</t:mo></t:msup></t:mrow></t:msub><t:msub><t:mi mathvariant=\"script\">B</t:mi><t:mrow><t:msub><t:mi>a</t:mi><t:mn>2</t:mn></t:msub><t:mo stretchy=\"false\">(</t:mo><t:mn>1320</t:mn><t:mo stretchy=\"false\">)</t:mo><t:mi>π</t:mi></t:mrow></t:msub></t:math> for the pure <z:math xmlns:z=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><z:mi>ρ</z:mi><z:mo stretchy=\"false\">(</z:mo><z:mn>2</z:mn><z:mi>D</z:mi><z:mo stretchy=\"false\">)</z:mo></z:math> state is about 2 orders of magnitude smaller than the experimental value. To resolve this discrepancy and decipher the nature of <db:math xmlns:db=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><db:mi>Y</db:mi><db:mo stretchy=\"false\">(</db:mo><db:mn>2044</db:mn><db:mo stretchy=\"false\">)</db:mo></db:math>, this work proposes an <hb:math xmlns:hb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><hb:mrow><hb:mi>S</hb:mi><hb:mtext>−</hb:mtext><hb:mi>D</hb:mi></hb:mrow></hb:math> mixing scheme to reanalyze the cross section of <jb:math xmlns:jb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><jb:msup><jb:mi>e</jb:mi><jb:mo>+</jb:mo></jb:msup><jb:msup><jb:mi>e</jb:mi><jb:mo>−</jb:mo></jb:msup><jb:mo stretchy=\"false\">→</jb:mo><jb:msub><jb:mi>a</jb:mi><jb:mn>2</jb:mn></jb:msub><jb:mo stretchy=\"false\">(</jb:mo><jb:mn>1320</jb:mn><jb:mo stretchy=\"false\">)</jb:mo><jb:mi>π</jb:mi></jb:math>, and finds that the aforementioned branching ratio discrepancy can be resolved. Our results show that the <ob:math xmlns:ob=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ob:mi>Y</ob:mi><ob:mo stretchy=\"false\">(</ob:mo><ob:mn>2044</ob:mn><ob:mo stretchy=\"false\">)</ob:mo></ob:math> structure can be reproduced by introducing four theoretically predicted <sb:math xmlns:sb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><sb:mrow><sb:mi>S</sb:mi><sb:mtext>−</sb:mtext><sb:mi>D</sb:mi></sb:mrow></sb:math> mixing <ub:math xmlns:ub=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ub:mi>ρ</ub:mi></ub:math> meson states <wb:math xmlns:wb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><wb:msubsup><wb:mi>ρ</wb:mi><wb:mrow><wb:mn>3</wb:mn><wb:mi>S</wb:mi><wb:mo>−</wb:mo><wb:mn>2</wb:mn><wb:mi>D</wb:mi></wb:mrow><wb:mo>′</wb:mo></wb:msubsup></wb:math>, <yb:math xmlns:yb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><yb:msubsup><yb:mi>ρ</yb:mi><yb:mrow><yb:mn>3</yb:mn><yb:mi>S</yb:mi><yb:mo>−</yb:mo><yb:mn>2</yb:mn><yb:mi>D</yb:mi></yb:mrow><yb:mrow><yb:mo>′′</yb:mo></yb:mrow></yb:msubsup></yb:math>, ρ</ac:mi>4</ac:mn>S</ac:mi>−</ac:mo>3</ac:mn>D</ac:mi></ac:mrow>′</ac:mo></ac:msubsup></ac:math>, and <cc:math xmlns:cc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><cc:msubsup><cc:mi>ρ</cc:mi><cc:mrow><cc:mn>4</cc:mn><cc:mi>S</cc:mi><cc:mo>−</cc:mo><cc:mn>3</cc:mn><cc:mi>D</cc:mi></cc:mrow><cc:mrow><cc:mo>′′</cc:mo></cc:mrow></cc:msubsup></cc:math> as intermediate resonances, in which dominant contribution arises from <ec:math xmlns:ec=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ec:msubsup><ec:mi>ρ</ec:mi><ec:mrow><ec:mn>3</ec:mn><ec:mi>S</ec:mi><ec:mo>−</ec:mo><ec:mn>2</ec:mn><ec:mi>D</ec:mi></ec:mrow><ec:mrow><ec:mo>′′</ec:mo></ec:mrow></ec:msubsup></ec:math> and their inference effect is also significant. Furthermore, we reanalyzed five additional isospin vector processes <gc:math xmlns:gc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><gc:msup><gc:mi>e</gc:mi><gc:mo>+</gc:mo></gc:msup><gc:msup><gc:mi>e</gc:mi><gc:mo>−</gc:mo></gc:msup><gc:mo stretchy=\"false\">→</gc:mo><gc:mi>ω</gc:mi><gc:msup><gc:mi>π</gc:mi><gc:mn>0</gc:mn></gc:msup></gc:math>, <jc:math xmlns:jc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><jc:msup><jc:mi>e</jc:mi><jc:mo>+</jc:mo></jc:msup><jc:msup><jc:mi>e</jc:mi><jc:mo>−</jc:mo></jc:msup><jc:mo stretchy=\"false\">→</jc:mo><jc:msub><jc:mi>f</jc:mi><jc:mn>1</jc:mn></jc:msub><jc:mo stretchy=\"false\">(</jc:mo><jc:mn>1285</jc:mn><jc:mo stretchy=\"false\">)</jc:mo><jc:msup><jc:mi>π</jc:mi><jc:mo>+</jc:mo></jc:msup><jc:msup><jc:mi>π</jc:mi><jc:mo>−</jc:mo></jc:msup></jc:math>, <oc:math xmlns:oc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><oc:msup><oc:mi>e</oc:mi><oc:mo>+</oc:mo></oc:msup><oc:msup><oc:mi>e</oc:mi><oc:mo>−</oc:mo></oc:msup><oc:mo stretchy=\"false\">→</oc:mo><oc:msup><oc:mi>π</oc:mi><oc:mo>+</oc:mo></oc:msup><oc:msup><oc:mi>π</oc:mi><oc:mo>−</oc:mo></oc:msup></oc:math>, <rc:math xmlns:rc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><rc:msup><rc:mi>e</rc:mi><rc:mo>+</rc:mo></rc:msup><rc:msup><rc:mi>e</rc:mi><rc:mo>−</rc:mo></rc:msup><rc:mo stretchy=\"false\">→</rc:mo><rc:mi>ρ</rc:mi><rc:mi>η</rc:mi></rc:math>, and <uc:math xmlns:uc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><uc:msup><uc:mi>e</uc:mi><uc:mo>+</uc:mo></uc:msup><uc:msup><uc:mi>e</uc:mi><uc:mo>−</uc:mo></uc:msup><uc:mo stretchy=\"false\">→</uc:mo><uc:msup><uc:mi>η</uc:mi><uc:mo>′</uc:mo></uc:msup><uc:msup><uc:mi>π</uc:mi><uc:mo>+</uc:mo></uc:msup><uc:msup><uc:mi>π</uc:mi><uc:mo>−</uc:mo></uc:msup></uc:math> based on the same <xc:math xmlns:xc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><xc:mrow><xc:mi>S</xc:mi><xc:mtext>−</xc:mtext><xc:mi>D</xc:mi></xc:mrow></xc:math> mixing framework, and simultaneously reproduced their experimental cross section data. This work provides a unified framework to elucidate all observed <zc:math xmlns:zc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><zc:mi>ρ</zc:mi></zc:math>-like structures near 2 GeV in the <bd:math xmlns:bd=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><bd:msup><bd:mi>e</bd:mi><bd:mo>+</bd:mo></bd:msup><bd:msup><bd:mi>e</bd:mi><bd:mo>−</bd:mo></bd:msup></bd:math> annihilation processes, and suggests that the <dd:math xmlns:dd=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><dd:mrow><dd:mi>S</dd:mi><dd:mtext>−</dd:mtext><dd:mi>D</dd:mi></dd:mrow></dd:math> mixing effect may be crucial for understanding the mass spectrum and decay behaviors of the higher <fd:math xmlns:fd=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><fd:mi>ρ</fd:mi></fd:math> meson states.","PeriodicalId":20167,"journal":{"name":"Physical Review D","volume":"35 1","pages":""},"PeriodicalIF":5.3000,"publicationDate":"2025-10-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Decoding the role of ρ mesonic states for elucidating the e+e−→a2(1320)π data and other reactions\",\"authors\":\"Qin-Song Zhou, Zi-Yue Bai, Jun-Zhang Wang, Hao Xu, Xiang Liu\",\"doi\":\"10.1103/pdfh-mk79\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Recently, the BESIII Collaboration observed a ρ</a:mi></a:math>-like structure <c:math xmlns:c=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><c:mi>Y</c:mi><c:mo stretchy=\\\"false\\\">(</c:mo><c:mn>2044</c:mn><c:mo stretchy=\\\"false\\\">)</c:mo></c:math> in <g:math xmlns:g=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><g:msup><g:mi>e</g:mi><g:mo>+</g:mo></g:msup><g:msup><g:mi>e</g:mi><g:mo>−</g:mo></g:msup><g:mo stretchy=\\\"false\\\">→</g:mo><g:msub><g:mi>a</g:mi><g:mn>2</g:mn></g:msub><g:mo stretchy=\\\"false\\\">(</g:mo><g:mn>1320</g:mn><g:mo stretchy=\\\"false\\\">)</g:mo><g:mi>π</g:mi></g:math>, suggesting that <l:math xmlns:l=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><l:mi>Y</l:mi><l:mo stretchy=\\\"false\\\">(</l:mo><l:mn>2044</l:mn><l:mo stretchy=\\\"false\\\">)</l:mo></l:math> may be a candidate of vector meson <p:math xmlns:p=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><p:mi>ρ</p:mi><p:mo stretchy=\\\"false\\\">(</p:mo><p:mn>2</p:mn><p:mi>D</p:mi><p:mo stretchy=\\\"false\\\">)</p:mo></p:math> by comparing resonance parameters. However, the theoretical prediction for the combined branching ratio <t:math xmlns:t=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><t:msub><t:mi mathvariant=\\\"normal\\\">Γ</t:mi><t:mrow><t:msup><t:mi>e</t:mi><t:mo>+</t:mo></t:msup><t:msup><t:mi>e</t:mi><t:mo>−</t:mo></t:msup></t:mrow></t:msub><t:msub><t:mi mathvariant=\\\"script\\\">B</t:mi><t:mrow><t:msub><t:mi>a</t:mi><t:mn>2</t:mn></t:msub><t:mo stretchy=\\\"false\\\">(</t:mo><t:mn>1320</t:mn><t:mo stretchy=\\\"false\\\">)</t:mo><t:mi>π</t:mi></t:mrow></t:msub></t:math> for the pure <z:math xmlns:z=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><z:mi>ρ</z:mi><z:mo stretchy=\\\"false\\\">(</z:mo><z:mn>2</z:mn><z:mi>D</z:mi><z:mo stretchy=\\\"false\\\">)</z:mo></z:math> state is about 2 orders of magnitude smaller than the experimental value. To resolve this discrepancy and decipher the nature of <db:math xmlns:db=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><db:mi>Y</db:mi><db:mo stretchy=\\\"false\\\">(</db:mo><db:mn>2044</db:mn><db:mo stretchy=\\\"false\\\">)</db:mo></db:math>, this work proposes an <hb:math xmlns:hb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><hb:mrow><hb:mi>S</hb:mi><hb:mtext>−</hb:mtext><hb:mi>D</hb:mi></hb:mrow></hb:math> mixing scheme to reanalyze the cross section of <jb:math xmlns:jb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><jb:msup><jb:mi>e</jb:mi><jb:mo>+</jb:mo></jb:msup><jb:msup><jb:mi>e</jb:mi><jb:mo>−</jb:mo></jb:msup><jb:mo stretchy=\\\"false\\\">→</jb:mo><jb:msub><jb:mi>a</jb:mi><jb:mn>2</jb:mn></jb:msub><jb:mo stretchy=\\\"false\\\">(</jb:mo><jb:mn>1320</jb:mn><jb:mo stretchy=\\\"false\\\">)</jb:mo><jb:mi>π</jb:mi></jb:math>, and finds that the aforementioned branching ratio discrepancy can be resolved. Our results show that the <ob:math xmlns:ob=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ob:mi>Y</ob:mi><ob:mo stretchy=\\\"false\\\">(</ob:mo><ob:mn>2044</ob:mn><ob:mo stretchy=\\\"false\\\">)</ob:mo></ob:math> structure can be reproduced by introducing four theoretically predicted <sb:math xmlns:sb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><sb:mrow><sb:mi>S</sb:mi><sb:mtext>−</sb:mtext><sb:mi>D</sb:mi></sb:mrow></sb:math> mixing <ub:math xmlns:ub=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ub:mi>ρ</ub:mi></ub:math> meson states <wb:math xmlns:wb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><wb:msubsup><wb:mi>ρ</wb:mi><wb:mrow><wb:mn>3</wb:mn><wb:mi>S</wb:mi><wb:mo>−</wb:mo><wb:mn>2</wb:mn><wb:mi>D</wb:mi></wb:mrow><wb:mo>′</wb:mo></wb:msubsup></wb:math>, <yb:math xmlns:yb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><yb:msubsup><yb:mi>ρ</yb:mi><yb:mrow><yb:mn>3</yb:mn><yb:mi>S</yb:mi><yb:mo>−</yb:mo><yb:mn>2</yb:mn><yb:mi>D</yb:mi></yb:mrow><yb:mrow><yb:mo>′′</yb:mo></yb:mrow></yb:msubsup></yb:math>, ρ</ac:mi>4</ac:mn>S</ac:mi>−</ac:mo>3</ac:mn>D</ac:mi></ac:mrow>′</ac:mo></ac:msubsup></ac:math>, and <cc:math xmlns:cc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><cc:msubsup><cc:mi>ρ</cc:mi><cc:mrow><cc:mn>4</cc:mn><cc:mi>S</cc:mi><cc:mo>−</cc:mo><cc:mn>3</cc:mn><cc:mi>D</cc:mi></cc:mrow><cc:mrow><cc:mo>′′</cc:mo></cc:mrow></cc:msubsup></cc:math> as intermediate resonances, in which dominant contribution arises from <ec:math xmlns:ec=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ec:msubsup><ec:mi>ρ</ec:mi><ec:mrow><ec:mn>3</ec:mn><ec:mi>S</ec:mi><ec:mo>−</ec:mo><ec:mn>2</ec:mn><ec:mi>D</ec:mi></ec:mrow><ec:mrow><ec:mo>′′</ec:mo></ec:mrow></ec:msubsup></ec:math> and their inference effect is also significant. Furthermore, we reanalyzed five additional isospin vector processes <gc:math xmlns:gc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><gc:msup><gc:mi>e</gc:mi><gc:mo>+</gc:mo></gc:msup><gc:msup><gc:mi>e</gc:mi><gc:mo>−</gc:mo></gc:msup><gc:mo stretchy=\\\"false\\\">→</gc:mo><gc:mi>ω</gc:mi><gc:msup><gc:mi>π</gc:mi><gc:mn>0</gc:mn></gc:msup></gc:math>, <jc:math xmlns:jc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><jc:msup><jc:mi>e</jc:mi><jc:mo>+</jc:mo></jc:msup><jc:msup><jc:mi>e</jc:mi><jc:mo>−</jc:mo></jc:msup><jc:mo stretchy=\\\"false\\\">→</jc:mo><jc:msub><jc:mi>f</jc:mi><jc:mn>1</jc:mn></jc:msub><jc:mo stretchy=\\\"false\\\">(</jc:mo><jc:mn>1285</jc:mn><jc:mo stretchy=\\\"false\\\">)</jc:mo><jc:msup><jc:mi>π</jc:mi><jc:mo>+</jc:mo></jc:msup><jc:msup><jc:mi>π</jc:mi><jc:mo>−</jc:mo></jc:msup></jc:math>, <oc:math xmlns:oc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><oc:msup><oc:mi>e</oc:mi><oc:mo>+</oc:mo></oc:msup><oc:msup><oc:mi>e</oc:mi><oc:mo>−</oc:mo></oc:msup><oc:mo stretchy=\\\"false\\\">→</oc:mo><oc:msup><oc:mi>π</oc:mi><oc:mo>+</oc:mo></oc:msup><oc:msup><oc:mi>π</oc:mi><oc:mo>−</oc:mo></oc:msup></oc:math>, <rc:math xmlns:rc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><rc:msup><rc:mi>e</rc:mi><rc:mo>+</rc:mo></rc:msup><rc:msup><rc:mi>e</rc:mi><rc:mo>−</rc:mo></rc:msup><rc:mo stretchy=\\\"false\\\">→</rc:mo><rc:mi>ρ</rc:mi><rc:mi>η</rc:mi></rc:math>, and <uc:math xmlns:uc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><uc:msup><uc:mi>e</uc:mi><uc:mo>+</uc:mo></uc:msup><uc:msup><uc:mi>e</uc:mi><uc:mo>−</uc:mo></uc:msup><uc:mo stretchy=\\\"false\\\">→</uc:mo><uc:msup><uc:mi>η</uc:mi><uc:mo>′</uc:mo></uc:msup><uc:msup><uc:mi>π</uc:mi><uc:mo>+</uc:mo></uc:msup><uc:msup><uc:mi>π</uc:mi><uc:mo>−</uc:mo></uc:msup></uc:math> based on the same <xc:math xmlns:xc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><xc:mrow><xc:mi>S</xc:mi><xc:mtext>−</xc:mtext><xc:mi>D</xc:mi></xc:mrow></xc:math> mixing framework, and simultaneously reproduced their experimental cross section data. This work provides a unified framework to elucidate all observed <zc:math xmlns:zc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><zc:mi>ρ</zc:mi></zc:math>-like structures near 2 GeV in the <bd:math xmlns:bd=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><bd:msup><bd:mi>e</bd:mi><bd:mo>+</bd:mo></bd:msup><bd:msup><bd:mi>e</bd:mi><bd:mo>−</bd:mo></bd:msup></bd:math> annihilation processes, and suggests that the <dd:math xmlns:dd=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><dd:mrow><dd:mi>S</dd:mi><dd:mtext>−</dd:mtext><dd:mi>D</dd:mi></dd:mrow></dd:math> mixing effect may be crucial for understanding the mass spectrum and decay behaviors of the higher <fd:math xmlns:fd=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><fd:mi>ρ</fd:mi></fd:math> meson states.\",\"PeriodicalId\":20167,\"journal\":{\"name\":\"Physical Review D\",\"volume\":\"35 1\",\"pages\":\"\"},\"PeriodicalIF\":5.3000,\"publicationDate\":\"2025-10-17\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physical Review D\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1103/pdfh-mk79\",\"RegionNum\":2,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"Physics and Astronomy\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physical Review D","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1103/pdfh-mk79","RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"Physics and Astronomy","Score":null,"Total":0}
Decoding the role of ρ mesonic states for elucidating the e+e−→a2(1320)π data and other reactions
Recently, the BESIII Collaboration observed a ρ-like structure Y(2044) in e+e−→a2(1320)π, suggesting that Y(2044) may be a candidate of vector meson ρ(2D) by comparing resonance parameters. However, the theoretical prediction for the combined branching ratio Γe+e−Ba2(1320)π for the pure ρ(2D) state is about 2 orders of magnitude smaller than the experimental value. To resolve this discrepancy and decipher the nature of Y(2044), this work proposes an S−D mixing scheme to reanalyze the cross section of e+e−→a2(1320)π, and finds that the aforementioned branching ratio discrepancy can be resolved. Our results show that the Y(2044) structure can be reproduced by introducing four theoretically predicted S−D mixing ρ meson states ρ3S−2D′, ρ3S−2D′′, ρ4S−3D′, and ρ4S−3D′′ as intermediate resonances, in which dominant contribution arises from ρ3S−2D′′ and their inference effect is also significant. Furthermore, we reanalyzed five additional isospin vector processes e+e−→ωπ0, e+e−→f1(1285)π+π−, e+e−→π+π−, e+e−→ρη, and e+e−→η′π+π− based on the same S−D mixing framework, and simultaneously reproduced their experimental cross section data. This work provides a unified framework to elucidate all observed ρ-like structures near 2 GeV in the e+e− annihilation processes, and suggests that the S−D mixing effect may be crucial for understanding the mass spectrum and decay behaviors of the higher ρ meson states.
期刊介绍:
Physical Review D (PRD) is a leading journal in elementary particle physics, field theory, gravitation, and cosmology and is one of the top-cited journals in high-energy physics.
PRD covers experimental and theoretical results in all aspects of particle physics, field theory, gravitation and cosmology, including:
Particle physics experiments,
Electroweak interactions,
Strong interactions,
Lattice field theories, lattice QCD,
Beyond the standard model physics,
Phenomenological aspects of field theory, general methods,
Gravity, cosmology, cosmic rays,
Astrophysics and astroparticle physics,
General relativity,
Formal aspects of field theory, field theory in curved space,
String theory, quantum gravity, gauge/gravity duality.